## Classical ElectrodynamicsProblems after each chapter |

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1.8 This expression for

1.8 This expression for

**energy**density is intuitively reasonable , since regions of high fields “ must ” contain considerable**energy**.Page

Bohr's formula ( 13.36 ) gives a reasonable description of the

Bohr's formula ( 13.36 ) gives a reasonable description of the

**energy**loss of relatively slow alpha particles and heavier nuclei .Page

Two substances having very different atomic structures will produce the same

Two substances having very different atomic structures will produce the same

**energy**loss for ultrarelativistic particles provided their densities are such ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

Greens theorem | 14 |

BoundaryValue Problems in Electrostatics I | 26 |

Copyright | |

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### Common terms and phrases

acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written